- #71
Son Goku
- 113
- 21
I would just note that due to the Reeh-Schlieder theorem there are no states of finite support with a well-defined particle number. This is what ultimately prevents the definition of a position operator for any type of particle in QFT.
For massive particles there is the Newton-Wigner operator which was a proposed attempt at a position operator, but these don't even commute at space like distances, nor are they elements of the observable algebra. They aren't true observables.
So for all particles in QFT there is really just the probability to excite local probes and no sensible notion of position.
For massive particles there is the Newton-Wigner operator which was a proposed attempt at a position operator, but these don't even commute at space like distances, nor are they elements of the observable algebra. They aren't true observables.
So for all particles in QFT there is really just the probability to excite local probes and no sensible notion of position.